JPH02264668A - Induction heater with closed magnetic path - Google Patents
Induction heater with closed magnetic pathInfo
- Publication number
- JPH02264668A JPH02264668A JP29958888A JP29958888A JPH02264668A JP H02264668 A JPH02264668 A JP H02264668A JP 29958888 A JP29958888 A JP 29958888A JP 29958888 A JP29958888 A JP 29958888A JP H02264668 A JPH02264668 A JP H02264668A
- Authority
- JP
- Japan
- Prior art keywords
- current
- heated
- eddy current
- soft magnetic
- induction heating
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
この発明は、金属などの場合に比べて表皮深さが深い場
合の誘導加熱、特にガンの温熱治療を1的とする人体の
誘導加熱において、被加熱物の深部にも比較的多くの発
熱を起こし、発熱の必要のない部位では発熱を起こさな
いようにする誘導加熱装置に関するものである。Detailed Description of the Invention (Industrial Application Field) This invention is applicable to induction heating for cases where the epidermis is deeper than that for metals, particularly for induction heating of the human body for the purpose of thermal treatment of cancer. This invention relates to an induction heating device that generates a relatively large amount of heat even in the deep part of an object to be heated, and that generates no heat in areas that do not require heat generation.
(従来の技術)
ガンの温熱治療を目的とする人体の電磁誘導加熱、すな
わち電磁誘導方式ハイパーサーミアが、近年注目されて
いる。これは人体に傷をつけずにガンを治療するという
点で、画期的なものである。(Prior Art) Electromagnetic induction heating of the human body for the purpose of thermal treatment of cancer, that is, electromagnetic induction hyperthermia, has been attracting attention in recent years. This is revolutionary in terms of treating cancer without causing any damage to the human body.
従来の技術として、第6図のように、被加熱物のまわり
にソレノイドを巻き、電流を流す装置がある。この装置
では、うず電流の持つ物理的な性質から、多くの発熱は
被加熱物の表面に集まり、被加熱物の深部に発熱を与え
るのが難しかった。すなわち、人体の深部に腫ggJ組
織がある場合は治療が困難であった。またこの場合、大
きな発熱を起こしてはならない組織、あるいは発熱の必
要が無い組織に発熱を与えないことも困難であった。As a conventional technique, as shown in FIG. 6, there is a device in which a solenoid is wound around an object to be heated and a current is passed therethrough. In this device, due to the physical properties of eddy current, much of the heat is collected on the surface of the object to be heated, making it difficult to generate heat deep within the object. That is, when the tumor ggJ tissue is located deep in the human body, it is difficult to treat it. In this case, it is also difficult to prevent heat from being applied to tissues that should not generate large amounts of heat or that do not need to generate heat.
これらの点を解決するものとして、特公報昭62−38
179号公報並びに昭62−197073号公報に記載
されたような装置が報告されている。これらの装置は、
先に述べたソレノイドによる装置に比べ、極めて有効な
ものである。しかしながら、特公報昭62−38179
号公報に記載された装置においては、ビオ−サバールの
法則およびうず電流の影響から、交番磁界は、交番磁界
を作るコイルや磁極から離れるにしたがって急激に減衰
する。そのため被加熱物には、中心部に比べて、コイル
や磁極付近で、かなり大きい発熱が起きるという欠点が
ある。この装置は、この点を解決するために、加熱中に
コイルや磁極の位置を変える工夫を行っている。また、
この装置は4つ以上のコイルを必要とするため、装置が
複雑になる。特公報昭62−197073号公報に記載
された装置は、被加熱物が均質な円筒の場合、その中央
部で部分的な温度上昇がみられるという計算結果が報告
されているが、実際の装置では、中央部に集中するはず
のうず電流が、コイルのある平面の上下に拡散してしま
う場合もある。As a solution to these points, Special Publication No. 62-38
Devices such as those described in Japanese Patent No. 179 and Japanese Patent No. 197073/1982 have been reported. These devices are
This is extremely effective compared to the solenoid-based device described above. However, Special Publication No. 62-38179
In the device described in the publication, due to the Biot-Savart law and the influence of eddy currents, the alternating magnetic field rapidly attenuates as it moves away from the coils or magnetic poles that create the alternating magnetic field. Therefore, the object to be heated has the disadvantage that considerably more heat is generated near the coil or magnetic pole than in the center. To solve this problem, this device is designed to change the positions of the coil and magnetic pole during heating. Also,
This device requires four or more coils, which adds complexity to the device. In the device described in Japanese Patent Publication No. 62-197073, calculation results have been reported that when the object to be heated is a homogeneous cylinder, a partial temperature rise is observed in the center. In this case, the eddy current that should be concentrated in the center may end up spreading above and below the plane where the coil is located.
(発明が解決しようとする課題)
本発明は、誘導加熱において、容易に被加熱物の深部に
も比較的多くの発熱を起こし、発熱の不用な部位は、発
熱を起こさないようにし、また少ないコイルの数で装置
を実現可能にしようとするものである。(Problems to be Solved by the Invention) The present invention is designed to easily generate a relatively large amount of heat even in the deep part of the object to be heated in induction heating, and to prevent and reduce heat generation in unnecessary parts. The idea is to make the device practical with the number of coils.
(課題を解決するための手段)
いま、その構成を説明すると、
(イ) 被加熱物1に、励磁コイル2奔巻いた環状の
軟質磁性体3をかぶせる。(Means for Solving the Problems) Now, the configuration will be explained: (a) An object to be heated 1 is covered with an annular soft magnetic material 3 around which two excitation coils are wound.
(0) 環状の軟質磁性体3のまわりを、被加熱物!
との間の少な(とも一部にすきまを作らずに、うず電流
または変位電流の流れうる物質4でおおう。(0) The object to be heated is placed around the annular soft magnetic material 3!
Cover the gap between the two parts with a material 4 through which eddy current or displacement current can flow, without creating any gaps.
(ハ) 交流電流を流す機能を有する、電流発生源5
を励磁コイル2に接続する。(c) Current generation source 5 having the function of flowing alternating current
is connected to the excitation coil 2.
以上のように装置する。なお、環状の軟質磁性体3は、
被加熱物1のまわりに閉じた交流磁路を形成する役目さ
え果たせば、形状は任意であり、途中で途切れていても
良(、また外輪、内輪とも、必ずしも真円でなくても良
い。励磁コイル2を巻いた環状Q軟質磁性体3の代わり
に、トロイダルコイル6を用いても良い。また、励磁コ
イル2及びトロイダルコイル6は、基本的には−っでよ
いが、増やしても構わない。うず電流または変位電流の
流れうる物質4は、被加熱物Iの表面の一部との間にす
きまが無ければ良く、環状の軟質磁性体3、励磁コイル
2、及びトロイダルコイル6との間にすきまがあっても
構わない。The device is set up as described above. Note that the annular soft magnetic body 3 is
As long as it fulfills the role of forming a closed alternating current magnetic path around the object to be heated 1, the shape may be arbitrary, and may be interrupted in the middle (also, both the outer ring and the inner ring do not necessarily have to be perfect circles). A toroidal coil 6 may be used instead of the annular Q soft magnetic body 3 around which the excitation coil 2 is wound.Furthermore, the number of excitation coils 2 and toroidal coils 6 may basically be -1, but they may be increased. No. The material 4 through which eddy current or displacement current can flow needs only to have no gap between it and a part of the surface of the object to be heated I, and between the annular soft magnetic material 3, the exciting coil 2, and the toroidal coil 6. It doesn't matter if there is a gap between them.
(作用)
上記のように装置し、励磁コイルに交流電流を流した場
合、うず電流または変位電流が環状の軟質磁性体3の周
りを、交流電流の周期で逆回転と逆回転を繰り返す。う
ず電流または変位電流の流れうる物質4を適切に選択す
ることで、うず電流の一部は、物質4から被加熱物1へ
と進入し、比較的深部を通って、再び物質4へと戻る。(Function) When the device is configured as described above and an alternating current is passed through the excitation coil, the eddy current or displacement current repeats reverse rotation and reverse rotation around the annular soft magnetic body 3 at the cycle of the alternating current. By appropriately selecting a substance 4 through which eddy current or displacement current can flow, a part of the eddy current enters the heated object 1 from the substance 4, passes through a relatively deep part, and returns to the substance 4 again. .
この現象は、被加熱物lの、うず電流または変位電流の
流れうる物質4ですきまなくおおわれた部分の、全てで
起こる。そのため、加温する対象lの深部には、うず電
流が集中して流れる。This phenomenon occurs in all parts of the object to be heated 1 that are tightly covered with the substance 4 through which eddy current or displacement current can flow. Therefore, eddy current flows in a concentrated manner in the deep part of the object l to be heated.
その結果、被加熱物lの深部にも比較的多くの発熱が起
こるのである。第5図のように、被加熱物が均質な円筒
で、筋肉と等価な電気的定数を有する場合、3次元場の
理論計算によると、中央部の発熱mは最大の発熱を有す
る部位のおよそ4分の1程度に達する。As a result, a relatively large amount of heat is generated even in the deep part of the object to be heated. As shown in Figure 5, when the object to be heated is a homogeneous cylinder with an electrical constant equivalent to that of a muscle, three-dimensional field theory calculations show that the heat generation m in the center is approximately It reaches about 1/4.
また、物質4ですきまなくおおわれていない被加熱物l
の一部分では、うずjf3流の進入がなく、発熱が起き
ない。In addition, the object to be heated that is not completely covered with substance 4
In a part of the area, the eddy JF3 flow does not enter and no heat is generated.
よって、発熱が不用である被加熱物lの部位では、物質
4ですきまなくおおわなければ良いまた、渦電流または
変位電流の流れうる物質4に液体を用いれば、それを入
れ換えてゆくことによって、被加熱物1の表面付近の温
度上昇を抑えることができる。Therefore, parts of the heated object l that do not need to generate heat need not be completely covered with the substance 4, and if a liquid is used as the substance 4 through which eddy current or displacement current can flow, by replacing it, A rise in temperature near the surface of the object to be heated 1 can be suppressed.
(実施例) 実施例1 第1図の様な構成で、 環状の軟質磁性体3はニッケル系フェライトを用いる。(Example) Example 1 With the configuration shown in Figure 1, The annular soft magnetic body 3 is made of nickel-based ferrite.
環状の磁性体3に励磁コイル2を数回巻(。The excitation coil 2 is wound several times around the annular magnetic body 3 (.
うず電流または変位電流を流しつる物質4は液体を用い
る。A liquid is used as the material 4 through which eddy current or displacement current flows.
電流発生源5は高周波電源とインピーダンス整合装置を
用いる。The current generation source 5 uses a high frequency power source and an impedance matching device.
被加熱物1の表面は、液体を適当な量で還流させること
により、冷却する。The surface of the object to be heated 1 is cooled by refluxing an appropriate amount of liquid.
実施例2
第2図は実施例2を示す
励磁コイル2を巻いた環状の軟質磁性体3の代わりにト
ロイダルコイル6を用いる。Embodiment 2 In FIG. 2, a toroidal coil 6 is used in place of the annular soft magnetic body 3 around which the excitation coil 2 is wound, which is shown in Embodiment 2.
実施例3
第3図は実施例3を示す
うず電流または変位電流の流れうる物質4が、被加熱物
1とすきまを作っていない部分を更に限定し、発熱の不
用な部位8での発熱を抑えることを狙っている。Embodiment 3 FIG. 3 shows Embodiment 3, in which the material 4 through which eddy current or displacement current can flow further limits the area where there is no gap with the object 1 to be heated, and heat generation is suppressed in areas 8 where heat generation is unnecessary. I'm aiming to suppress it.
この場合、環状の軟質磁性体3を用いた場合に限り、励
磁コイル2を、うず電流または変位電流の流れうる物質
4の外側に配置することもできる。In this case, only when an annular soft magnetic body 3 is used, the excitation coil 2 can be placed outside the substance 4 through which eddy current or displacement current can flow.
実施例4 第4図は実施例4を示す。Example 4 FIG. 4 shows Example 4.
発熱の不用な部位8での発熱を抑えるために被加熱物l
の表面の一部に絶縁物7を貼っている。In order to suppress heat generation in parts 8 that do not require heat generation, the object to be heated l
An insulator 7 is pasted on a part of the surface.
実施例5 実施例1において、 寸法、形状は、第5図に従い、軸対称とする。Example 5 In Example 1, The dimensions and shape are axially symmetrical according to FIG.
被加熱物lは筋肉と等価な電気的定数を有する物質(以
後ファントムと呼ぶ)を・選ぶ。As the object to be heated, a material (hereinafter referred to as a phantom) having an electrical constant equivalent to that of muscle is selected.
うず電流または変位電流の流れうる物質4は、0.02
[%]食塩水とする。The substance 4 through which eddy current or displacement current can flow is 0.02
[%] Use saline solution.
励磁コイル2は8回巻く。Excitation coil 2 is wound eight times.
高周波電源の周波数は13.56 [Mz]とする。The frequency of the high frequency power source is 13.56 [Mz].
実効値で0. 5 [A]の電流を励磁コイルに流すO
ファントムの表面は、食塩水を適当な量で還流させるこ
とにより、加泥中初期温度より1〜2ドC]低い温度に
保つ。Effective value is 0. A current of 5 [A] is passed through the excitation coil.O The surface of the phantom is kept at a temperature 1 to 2 degrees C] lower than the initial temperature during muddying by circulating an appropriate amount of saline solution.
なお、この場合の実験結果を、次の(発明の効果)のと
ころで述べる。Note that the experimental results in this case will be described in the next section (Effects of the Invention).
実施例6
実施例5において、実施例4で述べたように、ファント
ムの一部に絶縁物7を貼る。但し、絶縁物の材質は厚さ
1 [mm]の塩化ビニルとする。Example 6 In Example 5, as described in Example 4, the insulator 7 is attached to a part of the phantom. However, the material of the insulator is vinyl chloride with a thickness of 1 mm.
塩化ビニルを貼る部分は、円筒座標系でr=0、z=0
をファントムの中心としたときの、−600≦θ≦60
° −10[cm] <z<10 [cm]とする。The part where vinyl chloride is pasted is r = 0, z = 0 in the cylindrical coordinate system.
-600≦θ≦60 when is the center of the phantom
° −10 [cm] <z<10 [cm].
なお、この場合の実験結果を、次の(発明の効果)のと
ころで述べる。Note that the experimental results in this case will be described in the next section (Effects of the Invention).
(発明の効果) 実施例5、実施例6の実験値で発明の効果を立証する。(Effect of the invention) The experimental values of Examples 5 and 6 prove the effects of the invention.
実施例5の場合の1時間後の上昇温度の実験データを第
7図に示す。なお測定点は、円筒座標系でz=0、rw
oの点をファントムの中央として、z=o [cm]、
r=0. 2. 4. 6. 8 [cm]である。The experimental data of the temperature increase after 1 hour in the case of Example 5 is shown in FIG. The measurement point is z=0, rw in the cylindrical coordinate system.
With point o as the center of the phantom, z=o [cm],
r=0. 2. 4. 6. 8 [cm].
また、比較のため、第6図に示すような、ソレノイドを
用いた誘導加熱装置で同様の実験を行ったので、その実
験データを同時に示す。被加熱物lの表面は、加温中、
初期温度より2〜3[℃]低い温度に保ち、被加熱物1
及び励磁電流の周波数も同じにした。For comparison, a similar experiment was conducted using an induction heating device using a solenoid as shown in FIG. 6, and the experimental data is also shown. During heating, the surface of the object to be heated l is
The heated object 1 is kept at a temperature 2 to 3 [℃] lower than the initial temperature.
The frequency of the excitation current was also the same.
これを見ると本装置が深部にも比較的多(の発熱を与え
ていることが分かる。Looking at this, it can be seen that this device generates a relatively large amount of heat even deep within the body.
実施例6の場合の1時間後の温度上昇の結果を第8図に
示す。測定点はz=o [cm]、θ=O[0]、r=
0. 2. 4. 6. 8 [cm]と2−〇[cm
]、θ=180[’l、r=2. 4. 6゜8 [c
m]である。The results of the temperature rise after 1 hour in the case of Example 6 are shown in FIG. Measurement points are z=o [cm], θ=O[0], r=
0. 2. 4. 6. 8 [cm] and 2-0 [cm
], θ=180['l, r=2. 4. 6゜8 [c
m].
これを見ると塩化ビニルを貼った側の温度上昇が抑えら
れているのが分かる。Looking at this, you can see that the temperature rise on the side where PVC is pasted is suppressed.
以上の事から、容易に被加熱物の深部にも比較的多くの
発熱を起こし、発熱の不用な部位は、発熱を起こさない
ようにし、また少ないコイルの数で装置を実現可能にし
ようとするという、本発明の効果が立証できた。From the above, it is easy to generate a relatively large amount of heat even in the deep parts of the object to be heated, to prevent heat generation from unnecessary parts, and to make it possible to realize a device with a small number of coils. The effects of the present invention were verified.
第1図は本発明の斜視図
第2図は本発明の実施例2の斜視図
第3図は本発明の実施例3の上面図
第4図は本発明の実施例4の上面図
第5図は本発明の実施例5の断面図
第6図は、実験データの比較に用いた、ツレ/イドによ
る誘導加熱装置の断面図
第7図は、本発明及びツレ/イドによる誘導加熱装置の
実験データ
第8図は、本発明の他の実験データ
1、被加熱物
2、励磁コイル
3、環状の軟質磁性体
4、うず21流または変位?U流の流れうる物質5、電
流発生源
6、トロイダルコイル
7、絶縁物
8、発熱の不用な部位FIG. 1 is a perspective view of the present invention FIG. 2 is a perspective view of Embodiment 2 of the present invention FIG. 3 is a top view of Embodiment 3 of the present invention FIG. 4 is a top view of Embodiment 4 of the present invention Figure 6 is a cross-sectional view of an induction heating device using a thread/id, which was used for comparison of experimental data. Experimental data FIG. 8 shows other experimental data 1 of the present invention, object to be heated 2, excitation coil 3, annular soft magnetic body 4, eddy 21. Current or displacement? Substance 5 through which U current can flow, current generation source 6, toroidal coil 7, insulator 8, unnecessary parts that generate heat
Claims (1)
軟質磁性体3をかぶせる。 (ロ)環状の軟質磁性体3のまわりを、被加熱物1との
間の少なくとも一部にすきまを作らずに、うず電流また
は変位電流の流れうる物質4でおおう。 以上の構成を特徴とする閉磁路を持つ誘導加熱装置 2、励磁コイル2を巻いた環状の軟質磁性体3の代わり
に、トロイダルコイル6を用い た、請求項1の閉磁路を持つ誘導加熱装置 3、うず電流または変位電流の流れうる物質4が、被加
熱物1に比べて高温でない液体 である、請求項1または請求項2の閉磁路を持つ誘導加
熱装置 4、被加熱物1が生体である、請求項1または請求項2
または請求項3の誘導加熱装置 5、うず電流または変位電流の流れうる物質4が食塩水
である、請求項3または請求項4の閉磁路を持つ誘導加
熱装置 6、被加熱物1の表面の一部に貼るための絶縁物7を用
意する、請求項3または請求項4 の閉磁路を持つ誘導加熱装置[Claims] 1. (a) An annular soft magnetic material 3 around which an excitation coil 2 is wound is placed over the object to be heated 1. (b) Cover the annular soft magnetic material 3 with a material 4 through which eddy current or displacement current can flow, without creating a gap at least in part between it and the object to be heated 1. The induction heating device 2 with a closed magnetic path characterized by the above configuration, the induction heating device with a closed magnetic path according to claim 1, using a toroidal coil 6 instead of the annular soft magnetic material 3 around which the excitation coil 2 is wound. 3. The induction heating device 4 with a closed magnetic path according to claim 1 or 2, wherein the substance 4 through which an eddy current or displacement current can flow is a liquid whose temperature is lower than that of the object to be heated 1, and the object to be heated 1 is a living body. Claim 1 or Claim 2
Alternatively, the induction heating device 5 according to claim 3, the induction heating device 6 having a closed magnetic path according to claim 3 or 4, wherein the substance 4 through which eddy current or displacement current can flow is saline, The induction heating device with a closed magnetic path according to claim 3 or 4, wherein an insulator 7 is prepared for pasting on a part.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29958888A JPH02264668A (en) | 1988-11-29 | 1988-11-29 | Induction heater with closed magnetic path |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29958888A JPH02264668A (en) | 1988-11-29 | 1988-11-29 | Induction heater with closed magnetic path |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02264668A true JPH02264668A (en) | 1990-10-29 |
Family
ID=17874575
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29958888A Pending JPH02264668A (en) | 1988-11-29 | 1988-11-29 | Induction heater with closed magnetic path |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02264668A (en) |
-
1988
- 1988-11-29 JP JP29958888A patent/JPH02264668A/en active Pending
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